Q.A plane electromagnetic wave of frequency 25 MHz travels in free space along the x-direction. At a particular point in space and time, E=6.3 j^ V/m. What is B at this point?
Concept understanding — Electromagnetic Wave Relation
Electromagnetic Wave Relation: From Intuition to Precision
Imagine you're standing at the beach. You see a wave coming in — it has a certain speed, a certain distance between crests (wavelength), and a certain number of crests passing you per second (frequency). The faster the wave, the more crests pass you in a given time. That's the basic idea: speed = frequency × wavelength.
Now, light is also a wave — an electromagnetic wave. It doesn't need water or air; it travels through empty space at a staggering speed. The relation that governs all waves, including light, is:
v=fλ
where v is the wave speed, f is the frequency (in hertz, Hz), and λ (lambda) is the wavelength (in metres).
For electromagnetic waves in vacuum, this speed is a universal constant: c=3×108 m/s. So the relation becomes:
c=fλ
That's it. But let's unpack what this really means.
What is frequency? What is wavelength?
Frequency is how many complete wave cycles pass a fixed point in one second. A radio station broadcasting at 100 MHz means 100 million cycles per second. Higher frequency means more oscillations per second.
Wavelength is the distance between two consecutive crests (or troughs) of the wave. For visible light, wavelengths are tiny — around 400 to 700 nanometres (billionths of a metre).
The product fλ always equals the wave speed. So if frequency goes up, wavelength must go down to keep the product constant. This is why:
- Gamma rays have extremely high frequency and extremely short wavelength.
- Radio waves have low frequency and very long wavelength (metres to kilometres).
Both travel at the same speed c in vacuum.
Why does this matter for exams?
You'll use this relation in three main ways:
- Given frequency, find wavelength (or vice versa) — just rearrange: λ=fc or f=λc.
- Compare different regions of the electromagnetic spectrum — know that as frequency increases, wavelength decreases proportionally.
- Solve problems involving energy — because photon energy E=hf (where h is Planck's constant), the wave relation links energy to wavelength: E=λhc.
A common mistake: using c=fλ for waves in a medium (like glass or water). In a medium, the speed is less than c, so the wavelength changes but frequency stays the same. The relation v=fλ still holds, but v is now the speed in that medium.
A concrete example
A microwave oven operates at 2.45 GHz. What is its wavelength in vacuum?
f=2.45×109 Hz, c=3×108 m/s.
λ=fc=2.45×1093×108=0.122 m=12.2 cm
That's why the mesh on a microwave door has holes about 1–2 mm across — much smaller than 12 cm — so microwaves can't escape, but visible light (wavelength ~500 nm) passes through easily.
The big picture
The electromagnetic wave relation c=fλ is not a deep law of nature — it's a definitional consequence of what frequency and wavelength mean. But it's the single most useful tool for navigating the electromagnetic spectrum. Memorise it, understand it, and you'll be able to connect wave properties to energy, to colour, to radiation types, and to countless exam problems.
c=fλ — that's the relation. Everything else is just applying it.
The relation c = fλ connecting frequency and wavelength across the electromagnetic spectrum is introduced in the NCERT Class 12 Physics chapter on electromagnetic waves, tested in CBSE boards, JEE Main and NEET. Anyone searching "electromagnetic spectrum frequency wavelength relation class 12 physics" will find this wave-speed reasoning, including the medium-versus-vacuum distinction, matches the NCERT treatment.
Why this formula?
Electromagnetic Wave Relation: Why c=μ0ε01
Let's build this from first principles — not just memorising the formula, but understanding why light and all EM waves travel at this specific speed.
1. The Starting Point: Maxwell's Equations in Vacuum
In empty space (no charges, no currents), Maxwell's equations simplify to:
- Gauss's law for electricity: ∇⋅E=0
- Gauss's law for magnetism: ∇⋅B=0
- Faraday's law: ∇×E=−∂t∂B
- Ampère-Maxwell law: ∇×B=μ0ε0∂t∂E
The key insight: a changing electric field creates a magnetic field, and a changing magnetic field creates an electric field. This mutual induction is what sustains the wave.
2. Deriving the Wave Equation for E
Take the curl of Faraday's law:
∇×(∇×E)=∇×(−∂t∂B)=−∂t∂(∇×B)
Now use the vector identity: ∇×(∇×E)=∇(∇⋅E)−∇2E
Since ∇⋅E=0 in vacuum, this becomes:
−∇2E=−∂t∂(∇×B)
Substitute ∇×B from Ampère-Maxwell:
−∇2E=−∂t∂(μ0ε0∂t∂E)
Result: The electric field satisfies the wave equation:
∇2E=μ0ε0∂t2∂2E
3. Identifying the Wave Speed
Compare with the standard wave equation for any wave travelling at speed v:
∇2ψ=v21∂t2∂2ψ
Matching terms:
v21=μ0ε0⇒v=μ0ε01
This v is the speed of electromagnetic waves in vacuum — denoted c.
Why this is profound: The constants μ0 (permeability of free space) and ε0 (permittivity of free space) come from static electricity and magnetism. Yet their combination gives the speed of light — showing light is an electromagnetic wave.
4. The Magnetic Field Follows Suit
Exactly the same derivation starting from Ampère-Maxwell law gives:
∇2B=μ0ε0∂t2∂2B
So both E and B propagate at the same speed c.
5. The Crucial Relationship Between E and B
For a plane wave travelling in the x-direction:
- E oscillates along y: Ey=E0sin(kx−ωt)
- B oscillates along z: Bz=B0sin(kx−ωt)
From Faraday's law: ∂x∂Ey=−∂t∂Bz
Differentiating the wave forms:
kE0cos(kx−ωt)=ωB0cos(kx−ωt)
Since ω=ck, we get:
B0E0=kω=c
Key result: In vacuum, the magnitudes are related by:
E=cB
This means:
- E and B are perpendicular to each other and to the direction of propagation
- They are in phase (peaks and zeros occur together)
- The electric field is c times stronger than the magnetic field in SI units
6. Physical Intuition: Why This Speed?
Think of it this way:
- μ0 measures how strongly a current creates a magnetic field
- ε0 measures how strongly a charge creates an electric field
- Their product in the denominator means: the more "reluctant" space is to create fields, the slower the wave
If space were more "magnetic" (larger μ0) or more "electric" (larger ε0), EM waves would travel slower. The actual value c≈3×108 m/s emerges from the measured values of these constants.
Summary: The Core Relations
| Quantity | Formula | Why |
|---|---|---|
| Wave speed | c=μ0ε01 | From wave equation derived from Maxwell's equations |
| Field ratio | E=cB | From Faraday's law applied to plane waves |
| Direction | E⊥B⊥ propagation | From cross-product structure of Maxwell's equations |
Exam tip: Never just quote c=1/μ0ε0 — be ready to show it comes from taking curls of Maxwell's equations and identifying the wave equation form.
Concept: Electromagnetic Wave Relation — in free space, E and B are perpendicular, in phase, and related by c=E/B.
Step 1: The wave travels along x, and E is along j^. For a plane wave, B must be perpendicular to both the direction of propagation and E, so B is along k^.
Step 2: The magnitude relation is B=E/c, where c=3×108 m/s.
Step 3:
B=3×1086.3=2.1×10−8 T
Step 4: The direction is k^, so B=2.1×10−8 k^ T.
The magnetic field is 2.1×10−8 k^ T.
For an EM wave, E and B are perpendicular, in phase, and related by c=E/B. Here B=2.1×10−8 k^ T.
The key idea is that in a plane electromagnetic wave, the electric and magnetic fields are not independent — they are linked by Maxwell’s equations. For a wave traveling in free space, the ratio of their magnitudes is fixed by the speed of light, and their directions are perpendicular to each other and to the direction of propagation.
The wave moves along the x-direction. The electric field is given as E=6.3 j^ V/m, which points along the y-axis. For the wave to travel along x, the magnetic field must lie along the z-axis — that’s the only remaining perpendicular direction. The sign (whether +k^ or −k^) is determined by the fact that E×B must point in the direction of wave travel, which is +i^.
Let’s work through it step by step.
- Recall the fundamental relation In free space, the magnitudes of E and B in an electromagnetic wave satisfy
c=BE
where c=3×108 m/s is the speed of light. This comes directly from Maxwell’s equations — the wave equation for E and B gives the same speed c, and the fields are in phase with this ratio.
- Find the magnitude of B Given E=6.3 V/m, we have
B=cE=3×1086.3=2.1×10−8 T
- Determine the direction The wave travels along +i^. The electric field is along +j^. For the Poynting vector S=μ01(E×B) to point along +i^, we need E×B to be along +i^. Using the right-hand rule: j^×k^=i^. So B must be along +k^.
A quick check: if you ever forget the cross product direction, use the cyclic order x→y→z→x. Here x is propagation, y is E, so z must be B — and the sign follows from E×B∝propagation direction.
- Write the final vector Therefore,
B=2.1×10−8 k^ T
A common mistake is to forget that the frequency 25 MHz is irrelevant here — it only tells you the wave is in the radio band, but the relation E/B=c holds for any frequency in free space. Don’t let extra data distract you.
The magnetic field at that point is B=2.1×10−8 k^ T.
Method: The Right-Hand Rule and the Wave Relation for EM Waves
This problem uses the plane wave relation between electric and magnetic fields in free space, combined with the direction rule for electromagnetic waves.
Key Concept
For a plane EM wave traveling in free space:
- E, B, and the direction of propagation k^ are mutually perpendicular.
- The magnitudes are related by:
∣B∣=c∣E∣
where c=3×108 m/s.
Steps
-
Identify the direction of propagation
The wave travels along the x-direction. So k^=i^.
-
Identify the direction of E
Given: E=6.3 j^ V/m. So E points along +y.
-
Apply the right-hand rule
For a wave traveling in the +k^ direction:
k^=E^×B^
Here k^=i^, E^=j^.
Using i^=j^×B^, we get B^=k^ (the +z direction).
- Calculate the magnitude of B
B=cE=3×1086.3=2.1×10−8 T
- Write the final vector
B=2.1×10−8 k^ T
Quick Check
- Frequency 25 MHz is not needed here — it only confirms the wave is in the radio band, but the relation E=cB is frequency-independent in free space.
- The direction matches: x-propagation, y-electric field, z-magnetic field.
This is a classic problem from the Electromagnetic Waves chapter in NCERT Class 12 Physics. Here's a breakdown of the common mistakes students make on it, and how to avoid them.
🔍 The Correct Approach First
For an EM wave in free space:
- E, B, and direction of propagation are mutually perpendicular.
- Relation: ∣B∣=c∣E∣, where c=3×108 m/s.
- Direction: E×B gives the direction of wave travel.
Here:
- Wave travels along +x.
- E=6.3 j^ V/m (along +y).
- So B must be along +z (since j^×k^=i^).
Calculation:
∣B∣=3×1086.3=2.1×10−8 T
Final answer:
B=2.1×10−8 k^ T
✗ Common Mistake #1: Forgetting the Direction Rule
What students do wrong:
They calculate magnitude correctly but write B along +y or +x, or just give magnitude.
Why it happens:
They memorise "E and B are perpendicular" but don't apply the right-hand rule or the cross-product relation E×B∥propagation direction.
How to avoid:
- Always write: propagation direction = E×B direction.
- Use unit vectors: i^×j^=k^, j^×k^=i^, etc.
- Practice with all three axes.
✗ Common Mistake #2: Using Wrong Value of c
What students do wrong:
They use c=3×108 m/s but sometimes mistakenly use 3×108 km/s or forget the exponent.
Why it happens:
Rushing or not writing the formula clearly.
How to avoid:
- Always write c=3×108 m/s at the top.
- Double-check units: E in V/m, B in T.
- If frequency is given, it's a distractor — you don't need it here.
✗ Common Mistake #3: Using Frequency Unnecessarily
What students do wrong:
They try to use c=fλ or B=cE with frequency, leading to wrong numbers.
Why it happens:
The problem gives frequency (25 MHz) — students think it must be used.
How to avoid:
- Recognise: For a plane wave in free space, B=E/c is always true, independent of frequency.
- Frequency is only needed if they ask for wavelength or wave number.
✗ Common Mistake #4: Unit Confusion
What students do wrong:
They write B in Gauss instead of Tesla, or forget to convert MHz.
Why it happens:
Mixing CGS and SI units.
How to avoid:
- Stick to SI: E in V/m, B in T, c in m/s.
- 1 T = 104 G — but NCERT uses Tesla.
- Frequency in Hz: 25 MHz = 25×106 Hz (but again, not needed here).
✓ Quick Checklist to Avoid All Mistakes
| Step | Action |
|---|---|
| 1 | Identify propagation direction (given: +x) |
| 2 | Identify E direction (given: +y) |
| 3 | Use E×B∥ propagation to find B direction |
| 4 | Compute B=E/c with c=3×108 |
| 5 | Write final vector: magnitude + unit vector |
Final takeaway:
In free space, B=E/c always. The direction is the only tricky part — use the cross-product rule carefully.
- GUJCET 2026Set x1 markMCQQ.A charged particle oscillates about its mean equilibrium position with a frequency of 8×109 Hz. What is the frequency of the electromagnetic waves produced by the oscillator? (A) 4×109 Hz (B) 1.6×1010 Hz (C) 8×109 Hz (D) 2×109 Hz
›Reveal solutionSolution
[!TLDR]
Using the NCERT/CBSE list of insect-resistant crop varieties: X = flat bean, Y = Pusa A-4, Z = Aphids.
Concept
Under 'Strategies for Enhancement in Food Production', plant breeders release crop varieties resistant to specific insect pests. A standard table pairs each crop with its released variety and the pest it resists. This GSEB/NCERT-aligned question tests recall of three of those pairings.
Solution
- Row (i): Rape-seed mustard, variety Pusa Gaurav. This mustard variety is bred for resistance to the mustard aphid, so Z = Aphids.
- Row (ii): variety Pusa Sem 2, resisting Jassids. 'Pusa Sem' varieties belong to flat bean, so X = flat bean.
- Row (iii): Okra (bhindi) resisting shoot borer. The released okra variety here is Pusa A-4 (resistant to shoot and fruit borer), so Y = Pusa A-4.
Combining: X = flat bean, Y = Pusa A-4, Z = Aphids.
[!ANSWER]
(A) X - flat bean, Y - Pusa A-4, Z - Aphids
NoteThis solution was worked out by our team and independently cross-checked by a second solve. The official answer key on record for this question could not be confirmed, so please cross-verify with the official paper where possible.
- GSEB Higher Secondary Certificate (HSC) Examination 2026Set ANNUAL1 markMCQQ.The amplitude of the magnetic field of Electromagnetic wave is B_0 = 510 nT, then amplitude of electric field of Electromagnetic wave is E_0 = ___.(a) 143 V/m(b) 153 V/m(c) 135 V/m(d) 170 V/m
›Reveal solutionSolution
In an electromagnetic wave, the electric and magnetic field amplitudes are related by E_0 = c B_0, where c is the speed of light.
Given B_0 = 510 nT = 510 x 10^-9 T, c = 3 x 10^8 m/s.
E_0 = c B_0 = 3 x 10^8 x 510 x 10^-9 = 1530 x 10^-1 = 153 V/m.
✓Final answer(b) 153 V/m.
- GUJCET 2023Set 091 markMCQQ.If E and B represent electric and magnetic field vectors of electromagnetic wave, the direction of propagation of electromagnetic wave is along ______. (A) B (B) E (C) B×E (D) E×B
›Reveal solutionSolution
The Poynting direction E×B gives the wave's propagation direction.
Concept: In an electromagnetic wave, E, B, and the propagation direction form a right-handed triad, with propagation along E×B.
✓Final answer(D) E×B
ANSWER: (D)
- GSEB Higher Secondary Certificate (HSC) Examination 2023Set ANNUAL1 markMCQQ.For a given electromagnetic waves the magnitude of electric field is 6.6 V/m at a point in space. The magnitude of magnetic field at this point is ___ T.(a) 2.1 x 10^-8(b) 6.6 x 10^-8(c) 19.8 x 10^-8(d) 2.2 x 10^-8
›Reveal solutionSolution
In an EM wave the field magnitudes obey E = cB, so B = E/c = 6.6/(3x10^8) = 2.2 x 10^-8 T.
In an electromagnetic wave the electric and magnetic field amplitudes are related by E = c B.
So B = E/c = 6.6/(3 x 10^8) = 2.2 x 10^-8 T.
✓Final answer(d) 2.2 x 10^-8 T.
- GUJCET 2022Set 171 markMCQQ.A radio can tune into any station in the 6 MHz to 12 MHz band. What is the corresponding wavelength band? (c=3×108 m/s) (A) 40 m to 60 m (B) 25 m to 50 m (C) 20 m to 30 m (D) 10 m to 20 m
›Reveal solutionSolution
λ=c/f; higher frequency gives shorter wavelength.
Steps.
- At f=6 MHz: λ=6×1063×108=50 m.
- At f=12 MHz: λ=12×1063×108=25 m.
- Band: 25 m to 50 m.
✓Final answer(B) 25 m to 50 m
ANSWER: (B)
- GUJCET 2022Set 171 markMCQQ.A charged particle oscillates about its mean equilibrium position with a frequency of 109 Hz. What is the frequency of the electromagnetic waves produced by the oscillator? (A) 1018 Hz (B) 109 Hz (C) 10−9 Hz (D) 1010 Hz
›Reveal solutionSolution
An oscillating charge radiates EM waves at exactly its own oscillation frequency.
Concept. An accelerating/oscillating charge produces electromagnetic waves whose frequency equals the frequency of oscillation of the charge.
- Given oscillation frequency =109 Hz ⇒ EM wave frequency =109 Hz.
✓Final answer(B) 109 Hz
ANSWER: (B)
- GUJCET 2021Set 151 markMCQQ.A plane electromagnetic wave of frequency 25 MHz travels in free space along the X-direction. At a particular point in space and time, where B=2.1×10−8k^ T then find E at this point? (A) −2.1j^mV (B) 6.3j^mV (C) 4.2j^mV (D) −3.2j^mV
›Reveal solutionSolution
For an EM wave E=cB, with E,B and the propagation direction mutually perpendicular (E×B points along propagation).
Concept. E=cB and E^×B^=propagation^.
Solution. E=cB=(3×108)(2.1×10−8)=6.3 V/m. Wave goes along +i^; with B∥k^, we need E^×k^=i^, i.e. E^=j^. So E=6.3j^ V/m.
✓Final answer(B) 6.3j^mV
ANSWER: (B)
- GUJCET 2019Set 131 markMCQQ.At large distances from source E and B are in phase and the decrease in their magnitude is comparitively slower with distance r as per. (A) r2 (B) r−3 (C) r (D) r−1
›Reveal solutionSolution
Far from the source, radiated E and B are in phase and decrease as r1.
Concept: The radiation (far) field of an accelerating charge dominates at large distances because it decays only as 1/r, unlike the static (1/r2) or induction (1/r3) terms. This slow decay is why radiated energy reaches far away.
Steps:
- Near-field terms ∝r−2,r−3 die rapidly.
- The radiation term ∝r−1 survives, so E,B∝r−1.
✓Final answerOption (D) — r−1
ANSWER: (D)
- GSEB Higher Secondary Certificate (HSC) Examination 2019Set ANNUAL1 markMCQQ.The maximum value of E in an electromagnetic wave is equal to 1.8 Vm^-1. Thus the maximum value of B is ___.(a) 6 x 10^-8 T(b) 3 x 10^-6 T(c) 6 x 10^-9 T(d) 2 x 10^-10 T
›Reveal solutionSolution
In an electromagnetic wave, the peak electric and magnetic fields are related by B0=E0/c.
Given E0=1.8 V/m, c=3×108 m/s.
B0=cE0=3×1081.8=0.6×10−8=6×10−9 T.
✓Final answer(c) 6×10−9 T.
- GSEB Higher Secondary Certificate (HSC) Examination 2019Set ANNUAL1 markMCQQ.For a radiation of 6 GHz passing through air, the wave number (number of waves) per 1 m length is ___ (1 GHz = 10^9 Hz).(a) 5(b) 3(c) 20(d) 30
›Reveal solutionSolution
The number of complete waves per unit length (wave number in this sense) equals f/c, the reciprocal of wavelength.
Given f=6 GHz =6×109 Hz, c=3×108 m/s.
λ=c/f=6×1093×108=0.05 m.
Number of waves in 1 m =1/λ=1/0.05=20.
✓Final answer(c) 20.
- GSEB Higher Secondary Certificate (HSC) Examination 2018Set ANNUAL1 markMCQQ.In the region closer to the oscillating charges, the phase difference between E (vector) and B (vector) fields is ___ and their magnitude quickly decreases as ___ with distance r from the source.(a) 0, r^-1(b) pi/2, r^-3(c) pi/2, r^-1(d) 0, r^-3
›Reveal solutionSolution
Close to the oscillating charges (the near field), E and B are pi/2 out of phase and their amplitudes decrease steeply, as r^-3.
Near an oscillating charge (the induction/near-field zone, distances small compared with the wavelength):
- The electric and magnetic fields are out of phase by pi/2 (90 degree).
- Their magnitudes fall off quickly with distance, as r^-3.
(Only in the far radiation zone do E and B become in phase and decrease as 1/r, carrying energy away as the radiated wave.)
✓Final answer(b) pi/2, r^-3.
- GUJCET 2015Set C1 markMCQQ.To transmit a signal of 3 KHz frequency, the minimum length of antenna is _____ km (A) 25 (B) 20 (C) 50 (D) 75
›Reveal solutionSolution
[!TLDR]
λ=c/f=100 km; minimum antenna length =λ/4=25 km. Answer: (A).
Concept
To radiate a signal efficiently, an antenna should have a length of at least about a quarter of the signal wavelength, Lmin=λ/4, where λ=c/f (NCERT/CBSE communication systems).
Solution
Wavelength of the 3 kHz signal:
λ=fc=3×1033×108=105m=100km
Minimum antenna length:
Lmin=4λ=4100=25km
[!ANSWER]
(A) 25.
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